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Title: ON THE INDUCED CHARGE IN SEMICONDUCTOR DETECTORS

Abstract

The induced charge in an ionization chamber is usually represented by DELTA q = e DELTA x/d (1) or DELTA q = e DELTA V/V (2), where V = voltage across the device, d = spacing between electrodes, and DELTA V = potential difference between two points spaced DELTA x along the path of the charge e. Equation (1) is shown to be valid in the presence of a fixed space charge (depletion layer), while equation (2) is not. (D.L.C.)

Authors:
; ; ;
Publication Date:
Research Org.:
CISE, Milan
OSTI Identifier:
4749905
NSA Number:
NSA-17-014682
Resource Type:
Journal Article
Journal Name:
Nucl. Instr. Methods
Additional Journal Information:
Journal Volume: Vol: 21; Other Information: Orig. Receipt Date: 31-DEC-63
Country of Publication:
Country unknown/Code not available
Language:
English
Subject:
INSTRUMENTS AND INSTRUMENTATION; ELECTRIC CHARGES; ELECTRIC POTENTIAL; EQUATIONS; IONIZATION CHAMBERS; RADIATION DETECTORS; SEMICONDUCTORS

Citation Formats

Cavalleri, G, Fabri, G, Gatti, E, and Svelto, V. ON THE INDUCED CHARGE IN SEMICONDUCTOR DETECTORS. Country unknown/Code not available: N. p., 1963. Web. doi:10.1016/0029-554X(63)90106-X.
Cavalleri, G, Fabri, G, Gatti, E, & Svelto, V. ON THE INDUCED CHARGE IN SEMICONDUCTOR DETECTORS. Country unknown/Code not available. https://doi.org/10.1016/0029-554X(63)90106-X
Cavalleri, G, Fabri, G, Gatti, E, and Svelto, V. Tue . "ON THE INDUCED CHARGE IN SEMICONDUCTOR DETECTORS". Country unknown/Code not available. https://doi.org/10.1016/0029-554X(63)90106-X.
@article{osti_4749905,
title = {ON THE INDUCED CHARGE IN SEMICONDUCTOR DETECTORS},
author = {Cavalleri, G and Fabri, G and Gatti, E and Svelto, V},
abstractNote = {The induced charge in an ionization chamber is usually represented by DELTA q = e DELTA x/d (1) or DELTA q = e DELTA V/V (2), where V = voltage across the device, d = spacing between electrodes, and DELTA V = potential difference between two points spaced DELTA x along the path of the charge e. Equation (1) is shown to be valid in the presence of a fixed space charge (depletion layer), while equation (2) is not. (D.L.C.)},
doi = {10.1016/0029-554X(63)90106-X},
url = {https://www.osti.gov/biblio/4749905}, journal = {Nucl. Instr. Methods},
number = ,
volume = Vol: 21,
place = {Country unknown/Code not available},
year = {1963},
month = {1}
}